NMR studies of an oligonucleotide with an unusual structure induced by platinum anti-cancer drugs

Marked dependence on carrier-ligand bulk but not on carrier-ligand chirality of the duplex versus single-strand forms of a DNA oligonucleotide with a series of G-Pt(II)-G intrastrand cross-links modeling cisplatin-DNA adducts

The N7-Pt-N7 adjacent G,G intrastrand DNA cross-link responsible for cisplatin anticancer activity is dynamic, promotes local "melting" in long DNA, and converts many oligomer duplexes to single strands. For 5'-d(A1T2G3G4G5T6A7C8C9C10A11T12)-3' (G3), treatment of the (G3)2 duplex with five pairs of [LPt(H2O)2]2+ enantiomers (L = an asymmetric diamine) formed mixtures of LPt-G3 products (1 Pt per strand) cross-linked at G3,G4 or at G4,G5 in all cases. L chirality exerted little influence. For primary diamines L with bulk on chelate ring carbons (e.g., 1,2-diaminocyclohexane), the duplex was converted completely into single strands (G3,G4 coils and G4,G5 hairpins), exactly mirroring results for cisplatin, which lacks bulk. In sharp contrast, for secondary diamines L with bulk on chelate ring nitrogens (e.g., 2,2'-bipiperidine, Bip), unexpectedly stable duplexes having two platinated strands (even a unique G3,G4/G4,G5 heteroduplex) were formed. After enzymatic digestion of BipPt-G3 duplexes, the conformation of the relatively nondynamic G,G units was shown to be head-to-head (HH) by HPLC/mass spectrometric characterization. Because the HH conformation dominates at the G,G lesion in duplex DNA and in the BipPt-G3 duplexes, the stabilization of the duplex form only when the L nitrogen adducts possess bulk suggests that H-bonding interactions of the Pt-NH groups with the flanking DNA lead to local melting and to destabilization of oligomer duplexes. The marked dependence of adduct properties on L bulk and the minimal dependence on L chirality underscore the need for future exploration of the roles of the L periphery in affecting anticancer activity.

DNA interaction of dioxycyclobutenedione-(1,2-cyclohexanediamine) platinum(II) complex with potential anticancer activity

Dioxycyclobutenedione-(1,2-cyclohexanediamine)platinum(II), (R,R-DC-Pt) was found to have stronger cytotoxicity against six cancer cell lines than cisplatin and its DNA interactions was studied by calorimetric measurements, (13)C NMR. The binding specificity study of DNA base with R,R-DC-Pt was conducted by HPLC. To understand the molecular mechanism of R,R-DC-Pt with stronger cytotoxicity than that of cisplatin, we studied R,R-DC-Pt interaction with an oligonucleotide, d(ACCACGTGGT)(2), which contained c-H-ras gene encoding GGT by NMR spectroscopy. The oligomer DNA double helix was destroyed almost completely upon the R,R-DC-Pt binding. However under the same condition, the cisplatin binding with DNA was not so affected, and instead another conformation was formed, which suggests that larger damage to DNA can be induced by R,R-DC-Pt complex than that by cisplatin.

Mercury(II) Site-Selective Binding to a DNA Hairpin. Relationship of Sequence-Dependent Intra- and Interstrand Cross-Linking to the Hairpin-Duplex Conformational Transition

Hg(II) interacted site selectively with only one of three deoxyribooligonucleotides examined; these "oligos" each had a different number of unmatched T residues. Thus, Hg(II) formed an intrastrand T-Hg-T cross-link between the first and fourth T residues of the hairpin, d(GCGCTTTTGCGC) (T4). The DNA strand formed a loop around the Hg, as if the Hg atom had been lassoed. The interactions of Hg(II) with two other oligos, d(ATGGGTTCCCAT) (T2) and d(GCGCTTTGCGC) (T3), were less specific. Previously, we found that at high DNA and salt concentrations, T2 was a mixture of hairpin and duplex forms while T3 and T4 had the hairpin form; modeling studies showed that in the free T4 hairpin the two T's at the ends of the (T)(4) loop form a T.T wobble base pair. Only in T4 are the T residues positioned to form an intrastrand cross-link readily. The Hg(II)-oligo adducts formed as a function of added Hg(II) were investigated by titrations monitored by UV, CD, and (1)H NMR spectroscopy. The appearance of a new set of (1)H signals with the concomitant decay of the free oligo (1)H signals indicated that 1:1 Hg(II):T2, 1.5:1 Hg(II):T3, and 1:1 Hg(II):T4 adducts were formed with Hg(NO(3))(2). In H(2)O, these adducts all had spectra with very downfield signals for the exchangeable TN(3)H and GN(1)H groups, a characteristic of base-paired regions. All upfield N(3)H signals from the (T)(2) and (T)(3) sequences of the free oligo disappeared in the spectra of the 1:1 Hg(II):T2 and 1.5:1 Hg(II):T3 adducts. The disappearance of the NH signals, the UV spectral changes, and the stoichiometries (1:1 Hg(II):T2 and 1.5:1 Hg(II):T3) indicate that these adducts are duplexes containing two and three T-Hg-T interstrand cross-links for T2 and T3, respectively. The (1)H and (13)C signals of the 1:1 Hg(II):T4 adduct in D(2)O were nearly completely assigned by 2D NMR spectroscopy. The spectrum of the adduct in H(2)O had only two of the four original TN(3)H signals from the (T)(4) sequence present in the spectrum of T4; this result is consistent with the presence of a TN3-Hg-TN3 cross-link. The (13)C chemical shift changes upon Hg(II) binding indicated that the TN3-Hg-TN3 cross-link was between the T's at each end of the (T)(4) loop. The NOESY, CD, and UV spectra were all consistent with a hairpin conformation for the 1:1 Hg(II):T4 adduct. A hairpin conformation also appeared reasonable from molecular modeling calculations. In conclusion, the length of the central (T)(n)() sequence influenced the type of T-Hg-T cross-link formed and, in turn, the conformation of the adducts. For (T)(2) and (T)(3), interstrand T-Hg-T cross-linking favored the duplex form. In contrast, for (T)(4), intrastrand T-Hg-T cross-linking stabilized the hairpin form.

Similar conformations of hairpins with TTT and TTTT sequences: NMR and molecular modeling evidence for T.T base pairs in the TTTT hairpin

The conformations of the d[G(1)C(2)G(3)C(4)-T(a)T(b)T(c)T(d)-G(5)C(6)G(7)C(8)] (T4) and d[G(1)C(2)G(3)C(4)-T(a)T(b)T(c)-G(5)C(6)G(7)C(8)] (T3) DNA hairpins have been studied. The 1H and 31P signals of the two hairpins have been nearly completely assigned by means of two-dimensional NMR spectroscopy in D2O (NOESY (two-dimensional nuclear Overhauser effect and exchange spectroscopy) at mixing times of 5, 50, 100, 300 and 500 ms, double-quantum-filtered correlation spectroscopy (DQF-COSY) and 1H-31P reverse chemical shift correlation (RCSC), and one-dimensional NOE spectra in 90% H2O. Conformational analysis using distance geometry (DG), molecular mechanics (MM) and molecular dynamics (MD) gave model conformations, which were evaluated by comparison of experimental and simulated 2D NOESY spectra. For the T4 sequence in T4, both NMR data and modeling indicated a T(a).T(d) wobble base pair. Although two types of T(a).T(d) base pairs are possible, the one with T(a)NH-T(d)O4 and T(a)O2-T(d)NH H-bonds was calculated to be more stable. Because the T(a).T(d) base pair of T4 extends the stem, there are only two residues (T(b) and T(c) in the loop. Although there are three residues in the T3 loop, the T(c) base projects into the solvent. The resulting conformational models have very similar loop folding patterns (FP): the bases of the two adjacent residues that begin the loop [T(b)T(c) of T4 and T(a)T(b) or T3] have a minor groove/major groove orientation with the first residue each having a trans alpha torsion angle; and the phosphodiester group that links the residues at the 3' end of the loop and the 5' top of the stem [T(c)pT(d) of T4 and T(c)pG(5) of T3] has a gauche+, gauche+ zeta,alpha conformation with a trans gamma angle for the second residue in both. These or similar features appear to be present in most of the few other hairpins studied previously by conformational methods. Thus, we believe that the conformations of the loops in T3 and T4 hairpins have greater similarities than previously recognized.